“…To fix these coefficients, it is necessary to evaluate the Mellin-Barnes integral as a power series solution [24]. In particular, under the condition that the monodromy is irreducible (see 3 Due to the differential relation…”
Section: Mellin-barnes Integral Versus Horn Hypergeometric Functionmentioning
confidence: 99%
“…The sunrise or watermelon diagram (see Fig. 1) is one of the simplest Feynman diagrams which have been studied by the physics community as well as by mathematicians over the past fifty years [2][3][4][5][6][7][8][9][10][11][12][13][14]. This diagram has a few different representations.…”
Section: Introductionmentioning
confidence: 99%
“…1 It could also be rewritten in projective space [2,3]. where F and U are Symanzik polynomials [15] and α = L+1 j=1 α j .…”
A number of irreducible master integrals for L-loop sunrise and bubble Feynman diagrams with generic values of masses and external momenta are explicitly evaluated via the Mellin-Barnes representation.
“…To fix these coefficients, it is necessary to evaluate the Mellin-Barnes integral as a power series solution [24]. In particular, under the condition that the monodromy is irreducible (see 3 Due to the differential relation…”
Section: Mellin-barnes Integral Versus Horn Hypergeometric Functionmentioning
confidence: 99%
“…The sunrise or watermelon diagram (see Fig. 1) is one of the simplest Feynman diagrams which have been studied by the physics community as well as by mathematicians over the past fifty years [2][3][4][5][6][7][8][9][10][11][12][13][14]. This diagram has a few different representations.…”
Section: Introductionmentioning
confidence: 99%
“…1 It could also be rewritten in projective space [2,3]. where F and U are Symanzik polynomials [15] and α = L+1 j=1 α j .…”
A number of irreducible master integrals for L-loop sunrise and bubble Feynman diagrams with generic values of masses and external momenta are explicitly evaluated via the Mellin-Barnes representation.
“…In the paper [3] the Feynman integral of an eigenenergy diagram in a two-dimensional momentum space is investigated. Analogously one can investigate the Feynman integral of a ladder diagram of the sixth order (see [4]) which has the form…”
Section: Fuchsian Systems For Feynman Integralsmentioning
“…The strategy of such a kind of analysis is well know in the theory of special functions and the analytical theory of differential equations [12]. As is well known, any Feynman diagram satisfies a system of linear differential or difference equations with polynomial coefficients [13,14,15,16,17]. In modern mathematical language, such a system can be associated with the Gelfand-Karpanov-Zelevinskii functions or D-modules [18].…”
Section: Introduction: Feynman Diagrams and Special Functionsmentioning
Hypergeometric functions provide a useful representation of Feynman diagrams occuring in precision phenomenology. In dimensional regularization, the ε-expansion of these functions about d = 4 is required. We discuss the current status of differential reduction algorithms. As an illustration, we consider the construction of the all-order ε-expansion of the Appell hypergeometric function F 1 around integer values of the parameters and present an explicit evaluation of the first few terms.
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